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Page 376
... frame K ' , we expect the same physical laws to take the same form , OF λσ = 4π JA дха с σ = 1 ( 11.93 ) Using transformation ( 11.81 ) , we find that ( 11.93 ) can be expressed in terms of quantities in the original coordinate frame as ...
... frame K ' , we expect the same physical laws to take the same form , OF λσ = 4π JA дха с σ = 1 ( 11.93 ) Using transformation ( 11.81 ) , we find that ( 11.93 ) can be expressed in terms of quantities in the original coordinate frame as ...
Page 414
... frame where E = 0 if | B | > | E | , or B = 0 if | E | > | B | . In those coordinate frames the motion was relatively simple . If EB 0 , electric and magnetic fields will exist simultaneously in all Lorentz frames , the angle between ...
... frame where E = 0 if | B | > | E | , or B = 0 if | E | > | B | . In those coordinate frames the motion was relatively simple . If EB 0 , electric and magnetic fields will exist simultaneously in all Lorentz frames , the angle between ...
Page 514
... frame for our calculation and then transform to the laboratory at the end . Thus we will find that all but the final ... frame K ' , where the incident particle is at rest initially and the nucleus moves by with velocity vc , the ...
... frame for our calculation and then transform to the laboratory at the end . Thus we will find that all but the final ... frame K ' , where the incident particle is at rest initially and the nucleus moves by with velocity vc , the ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ